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Charm Physics Potential at BESIII Kanglin He Jan. 2004, Beijing hekl@ihep.ac.cn
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Outline Charm physics at threshold Absolute Branching Ratio Leptonic Decay and Decay Constant Semileptonic Decay and CKM Matrix Physics Beyond Standard Model D 0 D 0 Mixing CP violation Rare Charm Decay Summary
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Charm Physics at Threshold Charm threshold D physics @3.77GeV Ds physics @4.03GeV and @4.14GeV Why charm threshold Pair production of charmed D and Ds mesons With less or without background Take the advantage of BEPCII and BESIII Large data sample Better mass resolution and particle identification
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Charm Cross Section and Event Number for 1 yr running PhysicsC.M.S (GeV) Peak Lum. 10 33 cm -2 s -1 cross section (nb) Event Number D3.771.0~5~25M Ds4.030.6~0.32~1M Ds4.140.6~0.67~2M
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Absolute Branching Ratio Precision of Br(D 0 →Kπ), Br(D + →Kππ), Br(Ds→φπ) are normalization constants for Precision D, Ds physics Precision B physics Precision of Br(D 0 →Kπ), Br(D + →Kππ), Br(Ds→φπ) are needed for Decay constants Precision of CKM elements Model independent measurements at BESIII
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Tagging Technology(1) Pair Production of D and Ds mesons Large Brs (1~10%) of hadronic decay modes High tagged efficiency ~5M D tags, >0.2M Ds tags
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Tagging Technology(2) Beam Constrain Mass D + →Kππ Mode GeV/c 2
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Tagging Technology(3) Kinematic constrain for Double tags D + Double Tags D 0 Double Tags 80 pb -1 Monte Carlo DATA @3.77GeV
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Number of observed double tags in 5fp -1 Ds Data at 4.03GeV ~7000 double tags
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Tagging Technology(4) Number of expected double tags Number of expected single tags Combining the single tags and double tags
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Precision of Absolute Branching Ratio NowBESIII D 0 →Kπ~2.4%<1% D + →Kππ~6.6%<1% Ds→φπ~25%<2% Improvement after BESIII
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Leptonic Decay and Decay Constant
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Measurement of Decay constants at BESIII Take the advantage of running at charm threshold Pair production →Double tag method, model independent Take the advantage of BESIII detector High muon identification efficiency →suppress background Take the advantage of BEPCII Large data sample →reduce statistic error Information on the meson wave function Test lattice QCD Extract CKM elements |V cd |, |V cs | Theory→ extract |V td |, |V ts |
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Analysis Technique Double tag measurements Tagged D(s) with hadronic decay modes muon identification Absent of isolated photons Reconstruction of missing mass square →0
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Measurement of f Ds
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Precision of f D(s) (1) Major Uncertainty
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Precision of f D(s) (2) Great improvement after BESIII
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Semileptonic decay and CKM Matrix p D(s) Form Factor
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Measurement of CKM at BESIII Good performance of BESIII detector e/π/μ identification mass resolution Extract |V cd |, |V cs | Form factor shape and normalization Γ(q 2 ) describe the contribution of form factor, it was calculated from lattice QCD. The shape of form factor are helpful to theory. Extract the ratio of |V cd /V cs | Extract |V ub | from B physics →Theory
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Analysis Technique Hadronic tag PID U miss Signal Background (GeV/c)
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Precision of Branching Ratio of D 0, D + Semileptonic Decay PrecisionNowBESIII D 0 →K lν ~4.4%<1% D0→πlνD0→πlν ~17%<2% D + →K lν ~12%<2%
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Precision of CKM Form factor term ΔΓ/Γ , come from theory (Lattice QCD). Supposing ΔΓ/Γ ~3%, BESIII will get
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Form Factors From semileptonic decay of charm meson, dN/dq 2 will provide information on form factors (under studying)
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Physics Beyond Standard Model D 0 D 0 Mixing at ψ(3770) In SM, mixing is very small(10 -6 ). BESIII is sensitive to 10 -4 Possible to measure the phase shift CP violation in charm decays SM predicts the A CP may be as big as 10 -3. BESIII is sensitive to A CP >10 -2 Rare Charm Decay
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D 0 D 0 Mixing D 0 decays as D 0 Separate Mixing from DCS
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Mixing Phenomenology(1) Like the K 0 K 0 mixing, constructing D S and D L
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Experimental Situation x 0 0.1 0.2 0 -0.1 0.1 y x and y are in the orders of 10 -2 ─10 -1
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Mixing Phenomenology(2) DCS Mixing CF Measuring the Asymmetry of CP eigenstate (K + K - (+), K s ρ 0 (-) …) Supposing CP violation is small Possible to measure the phase shift
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Mixing at ψ(3770) The D 0 and D 0 are produced coherently in J PC =1 -- state DCSD (Double Cabbibo Suppressed Decay) contribution is 0 at ψ(3770) D 0 produced ~at rest, cannot measure ΔΓ (y) directly by using lifetime difference Useful for measuring r D
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Experimental Searching for D 0 D 0 Mixing Big challenge to PID (Kπchannel) Main backgrounds come from the double miss-PID Searching in semi-leptonic decay modes are experimental difficulty with 2 missing neutrino (hard to reduce background contribution to 10 -4 ) Monte Carlo study with different PID (TOF resolution)
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Detection efficiency vs TOF resolution
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Background rates vs TOF resolution
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Probing New Physics to r D ~10 -4 The detection efficiency is ~40%, ~20K events with D 0 →K + π - are expected to be found in 5fb -1 ψ(3770) data The background contamination rate is 0.1─0.5x10 -4 while the TOF resolution varies from 65ps to 100ps BESIII is sensitive to 10 -4 for the mixing rate if the TOF resolution is designed to be around 100ps.
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CP Violation at ψ(3770) Suppose Both D 0 decay to CP eigenstate f 1 and f 2. Any oberservations of CP( f 1 )=CP( f 2 ) at ψ(3770) are the direct evidence of CP Violation Several hundreds events with 100% CP eigenstate will be found in 5fb -1 ψ(3770) data. The sensitivity of direct CP violation is A CP ~10 -2 ─10 -1
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Rare Charm Decay The Up limit for most modes listed above are estimated in the range of 10 -6 ─10 -5, will update PDG data.
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Summary BESIII contributes to charm physics on Precision absolute branching ratio of charm mesons (<1% for D, <2% for Ds) Precision decay constants (2~3%) Precision CKM Matrix (<2%) Sensitive to r D ~10 -4 for mixing Sensitive to A CP ~10 -2 ─10 -1 for CP violation Set the up limit of branching ratio for most rare charm decays to 10 -6 ─10 -5 range And more, more,……
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Comparison of BES3, CLEO-c and B-factories On Charm physics topics Measurement B-factoriesCLEO-cBES3 —20041yr (2~3)%~0.6%<1% (3~5)%~0.7%<1% (5~10)%~1.9%<2% >10%~2.3%~3% (6~9)%~1.7%~2.5% Major ErrorSys.Stat. * D/Ds cross section over estimated by a factor of 2 this number need confirming
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Thank you ! 谢谢
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